Background of the Invention
[0001] This invention relates generally to optical materials and more particularly to a
method of forming bodies of optically transparent yttrium oxide.
[0002] As known in the art, there is a need for materials which are highly durable, and
which have substantial optical transparency in both the visible and infrared optical
bands. Applications for these materials include commercial systems such as metal vapor
lamps and optical windows, as well as, military systems, such as airborne optical
imaging systems. Optical imaging systems such as those found on an infrared heat seeking
missile, generally have one or more optical elements such as windows or domes which
are mounted on the external portion of the missile. These external elements are provided
to isolate the remaining optics of the imaging system from the external environment
through which the missile is flown. These external elements, therefore, must have
a particularly high degree of resistance to environmental exposures and must have
sufficient strength to protect the remaining components in the imaging system during
operation of the imaging system in addition to having the aforementioned substantial
transparency in the visible and/or infrared spectrums.
[0003] Several materials have been identified as potential candidates for these applications.
Each of these materials generally has a high degree of strength and is theoretically
capable of having a relatively high degree of infrared transparency, particularly
within the wavelength range of approximately 2 microns to 5 microns. One material
which is suitable in particular is yttrium oxide (Y₂O₃).
[0004] In addition to the aforementioned optical requirement for optical transparency in
the wavelength range of approximately 2 microns to 5 microns, it is also desirable
in certain applications that the optical element be transparent to wavelengths beyond
5 microns. For example, in missiles which are designed to travel at very high speeds
for long periods of time, a dome mounted on the front portion of such a missile will
reach elevated temperatures. A "hot" dome made of materials which do not transmit
to long wavelengths beyond 5 microns, for example, may produce undesirable emissions
resulting in increased system noise in the optical imaging system shielded by the
dome.
[0005] Moreover, associated with such a "hot" dome is a requirement that the material of
the dome withstand the thermal induced stresses created from the aerodynamic heating
of the surface thereof.
[0006] Some techniques for producing Y₂O₃ domes involve sintering to substantially full
density a Y₂O₃ body. In these techniques, sintering aids such as La are added up to
10% by weight to achieve the high density. The addition of these sintering aids has
one drawback. The sintering aids in a material such as Y₂O₃ will reduce its thermal
conductivity. Thus, reduced thermal conductivity will provide a concominant reduction
in thermal shock resistance of a dome. A hot dome, therefore, is susceptible to damage
due to the reduction in thermal shock resistance.
[0007] A technique has been described for producing high quality Y₂O₃ which is suitable
for the aforementioned applications. As described in U.S. Patent No. 4,761,390 Hartnett
et al., and assigned to the assignee of the present invention, relatively thick bodies
of Y₂O₃ are produced by densifying a consolidated body of substantially pure Y₂O₃
by sintering at an elevated temperature until the body has a closed porosity density
and then subjecting the closed porosity body to an elevated temperature and a simulatneous
elevated isostatic pressure until final densification (approximately 99.99% of theoretical)
has been achieved. The final densification step is followed by an annealing step to
restore the body to clear transparency. The clear body has an optical transparency
of greater than 73% over the wavelength range of 2-5 microns for samples having thickness
up to 0.375 inches. The body also has a high thermal conductivity and relative small
grain size and low coefficient of absorption. Thus, the material is a very desireable
material for the above applications.
[0008] One drawback, as discussed in the patent, is that during the final densification
step at the elevated temperature and elevated isostatic pressure, the yttria body
is exposed to a reducing environment. Thus oxygen is lost from the body and the samples
become non-stoichiometric. This oxygen defficiency results in a dark or black cast
to the material. Therefore, in the above patent, a post-densification annealing step
was performed to restore O₂ stoichiometry, thus removing the dark appearance after
the final densification step.
[0009] However, the samples occasionally have a slight yellow tinge after annealling which
degrades the visible transmittance properties. Y₂O₃ when subjected to a strongly oxidizing
atmosphere gains oxygen interstitials. It is possible that these interstitials could
cause this degradation in transmittance. Alternatively, it is possible that tungsten
(W) contamination from the element of the vacuum furnace used during the sintering
step could be present in the sample. This in turn would oxidize during annealling
and form WO₃, which is yellow.
[0010] It would be desireable, therefore, to eliminate the post densification annealling
step to prevent yellow tinge of the samples, while at the same time providing clear,
transparent Y₂O₃ and otherwise maintain all of the advantageous optical and material
properties described in the above-mentioned patent.
Summary of the Invention
[0011] In accordance with the present invention, a method of forming a transparent yttrium
oxide body comprises the steps of: providing a powder comprising of yttrium oxide
and consolidating said powder into a body of a predetermined size and shape. The
consolidated body is densified at an elevated temperature. Preferably, this temperature
is in the range of 1700-1900°C more preferable in the range of 1800°C to 1900°C for
period of time sufficient to densify the body to at least a closed porosity state.
Typically, a closed porosity state for such a body is at least 91% and preferably
94% to 96% of the theoretical density of the yttrium oxide. The sintered, closed porosity
body is then finally densified to substantially 100% of theoretical density by subjecting
said body to an elevated pressure preferably in the range of 25,000-30,000 psi for
a period of time of typically 1/2-10 hours at an elevated temperature preferable in
the range of 1700-1900°C. During final densification, the sintered body is disposed
adjacent a material which can supply an oxygen partial pressure to the body to maintain
the stoichiometry of the body. With this particular arrangement, a clear transparent
body of Y₂O₃ is provided after the final densification step without the need of further
temperature or pressure processing steps such as annealling. Also, the yellow tinge
occasionally provided with post annealled material is eliminated because the Y₂O₃
is no longer subjected to the relatively strong oxidizing environment typical of the
post-densification anneal. Thus, the anneal induced yellow tinge is eliminated, and
the cost of fabricating such a body is substantially reduced since an entire processing
step is eliminated. A sample of the body having a thickness of 2 mm has an optical
transparency of greater than about 75% over the wavelength range of about 2-6.5 microns
and has substantial optical transparency of at least 60% over wavelengths to at least
7 microns. Further, if the yttrium oxide body is substantially 100% yttrium oxide
(at least 99.9% yttrium oxide) as can be provided with this arrangement, then the
body will have a high thermal conductivity and, hence, a high thermal shock resistance.
[0012] In accordance with a further aspect of the present invention, a method of forming
a transparent yttrium oxide dome comprises the steps of providing a powder of yttrium
oxide having an average particle size of between 1 and 2.0 µm and having a maximum
agglomerated particle size of 10µm, with the yttrium oxide powder being substantially
99.99% yttrium oxide. The yttrium oxide powder is then consolidated into a dome of
predetermined size and shape by cold isostatic pressing the powder in a pressing mold
including a teflon-coated aluminum mandrel and a latex rubber or urethane rubber membrane
to define the shape of the dome. The powder is inserted into the mold and the assembly
is placed in an isostatic press and compacted at a pressure in the range of 25,000-30,000
psi. The compacted dome is then fired for a predetermined period of time at a temperature
in the range of 1350-1450°C until the dome is approximately 75% of theoretical maximum
density. This step is used primarily to drive off the binder vehicle and dispersant.
However, some densification of the compacted dome does occur during exposure to the
elevated temperature environment. The consolidated, dense dome is then densified to
approximately 95% of theoretical density or to provide the dome having a closed porosity
state by sintering the body in a vacuum furnace at a temperature in the range of 1700-1900°C.
The sintered densified dome is subjected to an elevated isostatic gas pressure of
25,000-30,000 psi and elevated temperature in the range of 1700-1900°C for a sufficient
period of time to provide the dome having a density which is substantially equal to
100% of the theoretical density for yttrium oxide. During this final densification
step, to prevent oxygen from being lost from the body, the body is disposed in a container
containing a suitable oxygen supplying media such as zirconium oxide (zirconia), yttrium
oxide (yttria), or magnesium oxide (magnesia) or another suitable media. A suitable
media is one which will not agglomerate during the densification step and can withstand
the high pressure and temperature encountered during the densification step, while
supplying an oxygen partial pressure. The presence of the oxygen supplying media will
establish a suitable 0₂ partial pressure about the Y₂O₃ body thereby maintaining the
body's O₂ stoichiometry. With this particular arrangement, a clear, transparent yttrium
oxide body is provided having a high thermal shock resistance, high optical transparency,
typically in excess of 75% between 3.0 and 5.0 microns for a 2 millimeter thick sample,
at least 60% transparency at wavelengths between 5 and 7 microns, and a relatively
low coefficient of absorption of less than about 0.1 cm ⁻¹ over the optical wavelength
band of 3 to 5 microns without the need for a post densification anneal to restore
O₂ stoichiometry.
Brief Description of the Drawings
[0013] The foregoing features of this invention, as well as the invention itself, may be
more fully understood from the following detailed description of the drawings in which:
FIG. 1 is a cross-sectional view of a container to house a Y₂O₃ sample during final
densification in accordance with the invention;
FIG. 2 is a cross-sectional view of an alternate container to house a Y₂O₃ sample
during final densification;
FIGS. 3A, 3B are plots of percent in-line optical transmittance as a function of wavelength
for a sample of yttrium oxide fabricated in accordance with the present invention,
as described in FIG. 1 compared to that described in the prior art over the visible
spectrum (FIG. 3A) and infrared spectrum (FIG. 3B); and
FIG. 4A, 4B are plots of percent in-line optical transmittance as a function of wavelength
for a sample of yttrium oxide fabricated in accordance with the invention as described
in conjunction with FIG. 2, over the visible spectrum (FIG. 4A) and infrared spectrum
(FIG. 4B);
FIG. 5 is a graph of thermal conductivity vs. temperature typical of the Y₂O₃ fabricated
in accordance with the present techniques.
Description of the Preferred Environments
[0014] Fabrication of an optically transparent body comprising yttrium oxide will now be
described. A powder comprising substantially 99.9% pure yttrium oxide preferable 99.99%
Y₂O₃ having an average particle size of 1.0µm - 2.0µm and having a maximum agglomerated
particle size of 10.0µm is provided. Yttrium oxide powder having the above-mentioned
specifications is provided as follows:
[0015] Yttrium oxide powder is obtained from Union Moly Corp., White Plains, N.Y. having
a surface area in the range of 20 to 45 m²/g and an average particle agglomerate size
of 1 to 3 micrometers. This powder is typically 99.99% pure yttrium oxide. The powder
is de-agglomerated, by ball milling in a polyethylene jug or a rubber lined milling
jar, for example, for a period of 5 to 24 hours using ceramic grinding media such
as zirconium oxide or yttrium oxide. After milling, the slurry is passed through a
400 mesh sieve to remove any large agglomerates and provide a de-agglomerated powder
having an average particle size between 1 and 2.0 micrometers and a maximum agglomerated
particle size of 10 micrometers. The powder may be further de-agglomerated by passing
the slurry through an ultrasonic horn to spray dry the powder. An organic binder vehicle
such as poly-vinylpyrolidone (typically PVP40/PVP10 in ratio of 4:1) up to 3% by weight
is added to the de-agglomerated powder before spray drying. A small amount of a dispersant
such as acetic acid is also added to the powder. The de-agglomerated powder having
the organic binder and dispersant is then passed through a spray drier which dries
the slurry at a rate of 1 liter/hr. The spray drying process step is generally used
for fabricating a nonplanar shaped body such as a hemispherical dome. It is generally
easier to have a free flowing powder to fill a nonplanar mold such as that used for
the hemispherical dome to insure a uniform density of the powder in the mold.
[0016] Once the powder having the above specified particle size is provided, the powder
is inserted into a pressing mold which will provide a rough body having substantially
the desired shape. For example, the pressing mold for a hemispherical dome may include
a teflon-coated aluminum mandrel to form the dome concave surface and a latex rubber
or urethane rubber membrane to define the convex surface of the dome. The mold is
filled with powder through a hole provided in the top portion of the mold and the
hole is sealed and air is evacuated from the mold. The assembly is then placed in
an isostatic press and compacted at an elevated pressure. Typically, an elevated pressure
in the range of about 25,000-30,000 psi is used.
[0017] After the rough dome has been removed from the mold, it is placed within a furnace
having an air atmosphere at a temperature in the range of 1350-1450°C to burnout the
binder vehicle previously provided in the mold. The body is kept at the elevated temperature
for a period of time of up to 90 minutes. Typically, the fired body has a density
of approximately 75% of theoretical density and has shrunk in size about 10 to 12
percent.
[0018] Final densification of the resulting green dome body is then provided in a two step
process. In the first step, the green dome is densified to a density of approximately
95% of theoretical density or at least to provide a body having a substantially closed
porosity state, that is having a density greater than about 91%. In a preferred embodiment,
this is accomplished by placing the body in a high vacuum tungsten furnace, which
is disposed at a temperature in the range of 1700-1900°C to sinter the body. A tungsten
furnace is used to reduce contamination of the Y₂O₃ body. In particular, a graphite
type furnace may cause severe loss of oxygen from the Y₂O₃ body as well as incorporation
of carbon into the body. The tungsten furnace is used to reduce the reduction of Y₂O₃
by chemical reaction with a reducing agent such as carbon present in graphite type
furnaces which are conventionally used during the sintering process. The body is maintained
at the elevated temperature typically for a time of 60 minutes or less. Preferably,
the body is enclosed or shielded by a Y₂O₃ container. During this sintering step,
there may be a slight tungsten film deposited over surface portions of the body particularly
if the body was not protected. This film is generally physically removed prior to
final densification. Other densification steps to achieve closed porosity may alternatively
be used such as hot-pressing.
[0019] The sintered body is then densified to substantially 100% of theoretical density
by subjecting the body to an elevated temperature in the range of 1700-1900°C and
an argon gas pressure of 25,000-30,000 psi for a period of time of 5 to 10 hours or
until substantially 100% of theoretical density for the body is achieved. Relatively,
short soaks at the maximum temperature are required, so long as the cycle time is
about 5 to 10 hours, at a minimum. The body is disposed in a container as shown in
FIGS. 1 or 2 when placed within the high temperature graphite furnace used for this
final densification step. After this densification treatment, the dome is fully dense
(99.9+% of theoretical density) and is clear, transparent.
[0020] Referring now to FIG. 1, a container 10 suitable to house a Y₂O₃ sample during the
final densification step which occurs over an elevated pressure and elevated temperature
is shown. The container 10 includes a crucible 12 here a cylinder having cylindrical
sidewalls 12a sealed to a bottom plate 12b. The crucible is preferable comprised of
either Y₂O₃ or ZrO₂ although other similar materials may be used. A setter plate 14
is disposed on the container 12 and is used to support sintered body 20 which is to
be finally densified into a clear optically transparent body. Disposed over the setter
plate 14 and shielding the body 20 is a dome 16 comprised of here Y₂O₃ or other suitable
material. Disposed in the remainder of the container 12 is an oxygen containing ceramic
media which is capable of withstanding the temperatures and pressures encountered
during final densification and which preferable will not agglomerate or densify itself
so that it may be easily removed after the final densification step.
[0021] Here suitable material for the media 22 is a zirconia grog (ZrO₂). Zirconium oxide
grog is characterized as a material with a large particle size. These coarse particles
are typically on the order of 100 µm to 500 µm and larger. During final densification,
some of the O₂ from the ZrO₂ will leave the grog, setting up an O₂ partial pressure
around the sample 20 thus inhibiting O₂ reduction or returning O₂ to the Y₂O₃ body
20. Thus, with the O₂ partial pressure the O₂ stoichiometry of the Y₂O₃ body is maintained
during the final densification step. This provides a body having a clear transparent
state. Other suitable media may include material grogs of yttrium oxide or magnesium
oxide for example.
[0022] Referring now to FIG. 2, an alternate container 10′ to house the Y₂O₃ dome during
final densification is shown. Container 10′ includes the crucible 12 as described
above. Here, however, the crucible 12 is filled with the media 22 as also described
above, and the dome is placed within the media without and Y₂O₃ bodies to shield the
dome sample 20 from the O₂ containing media.
[0023] After final densification with either type of container shown in FIGS. 1 and 2, the
dome is provided to a substantially clear, transparent state and may be ground and
polished using conventional techniques to provide a predetermined surface finish and
tolerance. For example, the body may be ground using fixed abrasive diamond tooling,
and a predetermined surface finish may be provided using alumina powder and high speed
lapping media.
[0024] Thus, a clear, transparent dome is provided without the need for any post densification
annealling cycles.
[0025] Referring now to FIGS. 3A and 3B, plots of in-line percent transmittance, uncorrected
for surface reflection losses for samples having a thickness of 2 mm are shown. In
FIG. 3A, percent transmittance is plotted against wavelength in nanometers, and in
FIG. 3B, percent transmittance is plotted against wavenumber in reciprocal centimeters.
Set forth in the Table are the process parameters for the two samples shown in FIGS.
3A and 3B. Curve 32 is for a sample having a thickness of 2 mm fabricated in accordance
with the teachings of U.S. Patent 4,761,390 using a post densification anneal at 1450
oC in air for approximately 5 hours. Curve 34 is for a sample also having a thickness
of 2 mm fabricated in accordance with the teachings of the present invention, using
an oxygen supplying media to maintain O₂ stoichiometry during the final densification
of the body.
[0026] Over the visible and short wavelength IR, spectrums of the present invention actually
had a slightly improved optical transparency. Over the IR spectrum from about 2.0
microns to 4.0 microns, the transparencies were substantially equal. Above 4.0 microns,
the transparency of the annealled sample is slightly better than that of the non-annealled
sample. Both slight differences are relatively unimportant and in general, this data
indicates that material provided by the present invention is as good as that provided
by the prior technique.
[0027] Referring now to FIGS. 4A, 4B, plots of in-line percent transmittance, uncorected
for surface reflection losses, for a sample having a thickness of 2 mm and fabricated
using the container of FIG. 2 are shown. In FIG. 4A, percent transmittance is plotted
against wavelength in nanometers, and in FIG. 4B, percent transmittance is plotted
against wave number in reciprocal centimeters. Curve 36 shows that over the visible,
and infrared spectrum, direct contact of the sintered body with the O₂ supplying media
also provides clear transparent material. The transparency measured over 0.6 µm to
7.0µm wavelength is substantially equivalent to that shown in FIGS, 3A, 3B for either
curve 32 or 34. Thus, either technique as described in conjunction with FIGS. 1 or
2 may be used to provide clear transparent material equivalent to that shown in the
abovementioned patent without the need for a post-anneal step.
TABLE
Curve |
Sample Thickness (mm) |
% T @ 4.0 µm |
Sinter ¹, ⁵ / |
Final Densification ¹,²,⁴ / |
|
|
Anneal |
|
|
|
Temp.(°C) |
Time(mins.) |
Temp.(°C) |
Time(hrs.) |
Temp.(°C) |
Time(hrs.) |
32 |
2.0 |
80 |
1890 |
30 |
1890 |
3 |
1450 |
5 |
34 |
2.0 |
79 |
1900 |
90 |
1900 |
4 |
|
|
36 |
2.0 |
79.2 |
1900 |
90 |
1900 |
4 ³/ |
|
|
¹ Times are for the dwell time at the max. temperature. |
² O₂ containing media was a ZrO₂ grog having a coarse grain, particle size of about
100 - 500 µm. |
³ ZrO₂ grog was in direct contact with the sample |
⁴ Pressure was 29,000 psi. |
⁵ Final sinter density was about 95%. |
[0028] Since the yttrium oxide bodies fabricated in accordance with the present invention
are substantially pure, that is comprise substantially 99.9% yttrium oxide, the body
comprised of yttrium oxide material has a high thermal conductivity and concominant
therewith, the yttrium oxide body will have a high thermal shock resistance, compared
to yttrium oxide bodies having dopant additives. The thermal conductivity characteristics,
typical of such samples of substantially pure Y₂O₃ are the same as mentioned in the
above-mentioned U.S. patent and are shown in FIG. 5.
[0029] Since the body is sintered only to achieve a closed porosity state (between about
91% to 96% of theoretical density) and accordingly, relatively short periods of time
and lower temperatures are used than those required by previous methods which attempted
to produce fully dense sintered bodies, the requirement for using dopant additives
to provide fully sintered bodies is eliminated. The use of a W (tungsten) heating
element furnace during the sintering cycle is seen as aiding the ability to sinter
the material to the closed porosity state without any dopant additives. Furthermore,
the W element aids in preventing contamination to the Y₂O₃ by the carbon reducing
generally associated with graphite heating elements. Moreover, the yttrium oxide bodies
fabricated in accordance with the present techniques are densified at significantly
lower temperatures and shorter duration exposure to environments which are believed
to increase degradation to the material and increase grain growth. Generally, material
fabricated in accordance with the present invention has an average grain size of about
150 microns.
[0030] Finally, the darkness generally associated with the body after final densification
is eliminated by using a container during such final densification step which contains
a media which provides an O₂ partial pressure to the body during final densification.
[0031] The calculated coefficient of absorption for material fabricated in accordance with
the present invention is expected to be less than about 0.1 cm⁻¹ as in the above U.S.
patent.
[0032] Thus, a simplified process which provides a Y₂O₃ body having all of the optical and
material advantages mentioned in the U.S. patent, but at a reduced processing cost
is provided.
[0033] Having described preferred embodiments in the invention, it will now become apparent
to one of the skill in the art that other embodiments incorporating their concepts
may be used. It is felt, therefore, that these embodiments should not be limited to
disclosed embodiments, but rather should be limited only to by the spirit and scope
of the appended claims.
1. A method of densifying a body having a substantially closed porosity density, comprised
of yttrium oxide, to substantially full density, comprises the step of:
densifying said closed porosity body by heating said body to an elevated temperature
at an elevated isostatic pressure until said body is substantially fully dense while
said body is disposed adjacent an oxygen supplying media which provides an oxygen
partial pressure to maintain O₂ stoichiometry in said body.
2. The method of Claim 1 wherein said media is selected from the group consisting
of zirconium oxide, magnesium oxide, and yttrium oxide.
3. The method of Claim 2 wherein said media is zirconium oxide.
4. A method of fabricating a body comprising yttrium oxide, comprises the steps of:
providing a starting powder of yttrium oxide;
compacting said yttrium oxide powder to form a body having a predetermined size and
shape;
sintering said compacted body at an elevated temperature to provide the body having
a closed porosity state; and
densifying said closed porosity body by heating said body to an elevated temperature
at an elevated pressure for a predetermined period of time until said body achieves
a density of substantially 100% of theoretical density while said body is disposed
adjacent a media which provides an oxygen partial pressure to restore or inhibit oxygen
reduction from the body.
5. The method of Claim 4 wherein said media is selected from the group consisting
of zirconium oxide, yttrium oxide, magnesium oxide.
6. The method of Claim 5 wherein said media is zirconium oxide.
7. The method of Claim 4 wherein said body is disposed in an enclosed container comprised
of a material selected for the group consisting of yttrium oxide, zirconium oxide,
magnesium oxide, the media is disposed adjacent said body and concludes a material
selected from the group consisting of zirconium oxide, yttrium oxide, or magnesium
oxide.
8. The method of Claim 7 wherein said body is disposed within the media and the media
is a grog of the selected material.
9. The method of Claim 7 wherein said body is at least partially shielded from the
media by a shield selected from the group consisting of zirconium oxide, yttrium oxide,
or magnesium oxide and said media is a grog of the selected material.
10. The method as recited in Claim 9 wherein the sintering step occurs in a high vacuum
tungsten heating element furnace.
11. The method as recited in Claim 10 wherein said densifying step occurs at a temperature
in the range of 1700°C to 1900°C at an elevated pressure in the range of 25,000 psi
to 30,000 psi.
12. The method as recited in Claim 11 wherein said temperature of the sintering step
is in the range of 1700°C to 1900°C.
13. The method as recited in Claim 12 wherein said temperature of the sintering step
is in the range of 1800°C to 1900°C.
14. A method of fabricating a body comprising yttrium oxide, comprises the steps of:
providing a yttrium oxide powder having an average particle size between 1 and 2.0
micrometers, and having a maximum agglomerated particle size of 10 micrometers;
consolidating said powder to provide a body having a density of about 75% of theoretical
density;
densifying the 75% dense body to a closed porosity state in a vacuum at a temperature
in the range of 1700-1900°C for a period of time at the maximum temperature of typically
30 minutes or less; and
densifying the closed porosity, sintered body to substantially 100% of theoretical
density by subjecting the body to a temperature in the range of 1700-1900°C at a pressure
in the range of 25,000-30,000 psi while said sintered body is disposed in a container
containing zirconium oxide which acts as a source of oxygen during the densification
step to maintain the stoichiometry of the yttrium oxide.
15. The method as recited in Claim 14 wherein after the densifying step occurs, the
body is removed from the container, and subjected to the step of grinding and polishing
the body to provide a predetermined surface finish.
16. The method of Claim 15 wherein said densifying step occurs at a temperature in
the range of about 1700°C to 1900°C.
17. A method of fabricating a non-planar body comprised of at least 99.9% yttrium
oxide having a transmittance of at least 75% over a wavelength range of 2.5 to 6.5
microns for a sample having a thickness of about 0.08 inches, comprises the steps
of:
providing a yttrium oxide powder having an average particle size of 1 to 2.0 micrometers
and having a maximum agglomerated particle size of 10 microns;
adding a binder vehicle and dispersant to the powder and spray drying the powder to
provide a free flowing powder;
directing the free flowing powder into a non-planar mold and subjecting the powder
in the non-planar mold to an isostatic pressure in the range of 25,000-30,000 psi;
removing the binder vehicle by subjecting the powder to a temperature in the range
of 1350-1450°C for a predetermined period of time in an atmosphere of air;
densifying the powder to a closed porosity state in a vacuum at a temperature in the
range of 1700-1900°C for a period of time at the maximum temperature of typically
30 minutes or less; and
densifying the closed porosity sintered body to substantially 100% of theoretical
density by subjecting the body to a temperature in the range of 1700-1900°C at a pressure
in the range of 25,000-30,000 psi until the body is substantially 100% of theoretical
density while said body is disposed adjacent zirconium oxide which provides an oxygen
partial pressure about said body during the densifying step.
18. The method of Claim 17 wherein said non-planar body is a hemispherical dome.
19. The method of Claim 18 wherein after the densifying step, the dome is subjected
to the step of grinding and polishing the dome surface until the surface is provided
with a predetermined surface finish.